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Takatani T, Hohenstein EG, Malagoli M, et al. Basis set consistent revision of the S22 test set of noncovalent interaction energies. J Chem Phys. 2010;132(14):144104doi: 10.1063/1.3378024.
Takatani, T., Hohenstein, E. G., Malagoli, M., Marshall, M. S., & Sherrill, C. D. (2010). Basis set consistent revision of the S22 test set of noncovalent interaction energies. The Journal of chemical physics, 132(14), 144104. https://doi.org/10.1063/1.3378024
Takatani, Tait, et al. "Basis set consistent revision of the S22 test set of noncovalent interaction energies." The Journal of chemical physics vol. 132,14 (2010): 144104. doi: https://doi.org/10.1063/1.3378024
Takatani T, Hohenstein EG, Malagoli M, Marshall MS, Sherrill CD. Basis set consistent revision of the S22 test set of noncovalent interaction energies. J Chem Phys. 2010 Apr 14;132(14):144104. doi: 10.1063/1.3378024. PMID: 20405982.
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J Chem Phys. 2010 Apr 14;132(14):144104. doi: 10.1063/1.3378024.

Basis set consistent revision of the S22 test set of noncovalent interaction energies.

The Journal of chemical physics

Tait Takatani, Edward G Hohenstein, Massimo Malagoli, Michael S Marshall, C David Sherrill

Affiliations

  1. Center for Computational Molecular Science and Technology, School of Chemistry and Biochemistry, Georgia Institute of Technology, Atlanta, Georgia 30332-0400, USA.

PMID: 20405982 DOI: 10.1063/1.3378024

Abstract

The S22 test set of interaction energies for small model complexes [Phys. Chem. Chem. Phys. 8, 1985 (2006)] has been very valuable for benchmarking new and existing methods for noncovalent interactions. However, the basis sets utilized to compute the CCSD(T) interaction energies for some of the dimers are insufficient to obtain converged results. Here we consistently extrapolate all CCSD(T)/complete basis set (CBS) interaction energies using larger basis sets for the CCSD(T) component of the computation. The revised values, which we designate S22A, represent the most accurate results to date for this set of dimers. The new values appear to be within a few hundredths of 1 kcal mol(-1) of the true CCSD(T)/CBS limit at the given geometries, but the former S22 values are off by as much as 0.6 kcal mol(-1) compared to the revised values. Because some of the most promising methods for noncovalent interactions are already achieving this level of agreement (or better) compared to the S22 data, more accurate benchmark values would clearly be helpful. The MP2, SCS-MP2, SCS-CCSD, SCS(MI)-MP2, and B2PLYP-D methods have been tested against the more accurate benchmark set. The B2PLYP-D method outperforms all other methods tested here, with a mean average deviation of only 0.12 kcal mol(-1). However, the consistent, slight underestimation of the interaction energies computed by the SCS-CCSD method (an overall mean absolute deviation and mean deviation of 0.24 and -0.23 kcal mol(-1), respectively) suggests that the SCS-CCSD method has the potential to become even more accurate with a reoptimization of its parameters for noncovalent interactions.

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